Department of Energy to conduct research focused on resolving the key technical issues that limited the deployment of efficient and extremely compact microtechnology based heat actuated absorption heat pumps and gas absorbers. Success in...
moreDepartment of Energy to conduct research focused on resolving the key technical issues that limited the deployment of efficient and extremely compact microtechnology based heat actuated absorption heat pumps and gas absorbers. Success in demonstrating these technologies will reduce the main barriers to the deployment of a technology that can significantly reduce energy consumption in the building, automotive and industrial sectors while providing a technology that can improve our ability to sequester CO 2 . The proposed research cost $939,477. $539,477 of the proposed amount funded research conducted at OSU while the balance ($400,000) was used at PNNL. The project lasted 42 months and started in April 2001. Recent developments at the Pacific Northwest National Laboratory and Oregon State University suggest that the performance of absorption and desorption systems can be significantly enhanced by the use of an ultra-thin film gas/liquid contactor. This device employs microtechnology-based structures to mechanically constrain the gas/liquid interface. This technology can be used to form very thin liquid films with a film thickness less then 100 microns while still allowing gas/liquid contact. According to the 1997 Residential Energy Consumption Survey (RECS), 56.6 million households were served by central (ducted) warm-air furnace systems. These systems consumed 3.31 Quads of energy (mostly natural gas and fuel oil) at a cost of $24.53 billion. The efficiency of a typical central furnace is assumed to be about 80%, while the Coefficient of Performance (COP) of an absorption heat pump is estimated to be about 1.2. Thus, the 25% savings associated with ducting losses, etc., coupled with the increase in equipment efficiency would combine to cut energy use in half, resulting in energy savings of 1.66 Quads valued at $12.26 billion per year. Central (ducted) heat pumps provided heating for 9.7 million households according to the 1997 RECS. These electrically-driven devices consumed 0.13 Quads (measured at the site) at a cost of $2.64 billion. According to figures presented in the 1997 Annual Energy Review, the combined conversion, transmission, and distribution efficiency for electricity was 30%. Thus, 0.13 Quads at the site is equivalent to 0.43 Quads at the source. Assuming a COP of 2.5 for an electrically-driven heat pump (compared to a COP of 1.2 for the absorption heat pump) and 25% savings for reduced ducting losses, etc., site energy use would increase from 0.13 Quads to 0.20 Quads. The absorption heat pump is not electrically-driven; so site and source energy are the same. Thus, the net source energy savings are 0.23 Quads per year. The cost of 0.20 Quads of fossil energy in the residential sector (based on RECS data for space heating) would be $1.50 billion, resulting in net energy dollar savings of $1.14 billion per year. Central (ducted) air conditioning systems (via heat pumps or AC only systems) were used in 47.5 million households according to the 1997 RECS, consuming 0.34 Quads of electricity (measured at the site) at a cost of $8.26 billion. This is equivalent to 1.13 Quads of source energy when energy electricity generation, transmission, and distribution losses are included. The absorption heat pump COP is only expected to be 0.65 in the cooling mode, compared to an assumed COP of 2.5 for the electrically-driven heat pump. Nevertheless, when coupled with 25% load savings for reduced ducting losses, etc., source energy consumption for the absorption heat pump is only 0.98 Quads, resulting in annual energy savings of 0.15 Quads. The 0.98 Quads of fossil energy is estimated to cost $7.26 billion in the residential sector (based on RECS data for space heating), resulting in annual dollar savings of $1.0 billion. The combined annual savings for central (ducted) heating and cooling systems are 2.04 Quads (source energy) and $14.4 billion. Site energy savings were estimated to be 0.47 Quads of electricity and 0.48 Quads of fossil energy. The latter is roughly 80% natural gas and 20% fuel oil. Air conditioning of automobiles is currently accomplished with vapor compression devices that are driven by shaft power generated by the auto's engine. With an IC engine efficiency of about 20% and an automotive vapor compression COP of 0.8, overall efficiency is poor. Absorption coolers offer significant performance improvement by avoiding the inefficiencies of IC engine shaft power. Conventional absorption-based cooling systems are too bulky for the automotive application, however, so development of a compact absorption cooling system is required to take advantage of the efficiency improvement opportunity. According to the Transportation Energy Data Book (Davis 1998), 130 million cars were driven 1.47 trillion miles or an average of 11,314 miles per car. The average speeds for the federal urban and highway driving cycles are 20 mph and 50 mph, respectively. Assuming that half of the annual mileage is accumulated at the urban rate and half at the highway rate, the total annual driving hours would be about 400. The number of air-conditioned driving hours would depend on climate and typical driving schedules. Lacking better data, air conditioning was assumed to be required half of the time. A passenger car cooling system is commonly sized to provide up to 2 tons (24,000 Btu/hour) of cooling. The cooling unit operates at capacity when bringing a car down from a "hot soak" condition to a comfortable operating temperature. At steady-state the required cooling capacity is much lower. This analysis assumes the air conditioner operates at full capacity for 20% of the cooling hours, but only 20% of capacity for the rest of the cooling hours, for an average capacity factor of 0.36 or average capacity of 0.72 tons or 8640 Btu/hour. Thus, the annual average cooling load served by the air conditioning system is 1.728 MMBtu With an IC engine efficiency of 0.20 and vapor compression COP of 0.8, the conventional automotive AC system consumes 10.8 MMBtu/year in the form of gasoline. The absorption cooler COP is estimated to be 0.5 in the automotive application. Its COP for the automotive application is less than for the space cooling application because the automotive condensing temperatures are generally higher. Although IC engine waste heat could provide part of the thermal input to the absorption cooler, the quantity available is not always adequate. This analysis assumes that all of the thermal input for the absorption cooler comes from combusting gasoline in a micro-channel combustor at an efficiency of 80% (i.e., 80% of the fuel's chemical energy is converted and transferred to the absorption cooler). Thus, the annual energy consumption for the absorption cooler is 4.32 MMBtu/year or a savings of 6.48 MMBtu/year. This is equivalent to 52 gallons of gasoline per year or a dollar savings of about $78 per year. If applied to the population of automobiles (130 million passenger cars), the total annual savings would be 0.84 Quads and $10.1 billion.. These figures do not include the potential impact of 69 million light trucks (pickups, vans, and utility vehicles). Nor do these figures consider the potential impact of enabling air conditioning in future electric, fuel cell, or hybrid vehicles where the shaft power demand of a conventional vapor compression unit would be a significant burden.